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Scattering angles

This differential cross section may be integrated over scattering angles to define an integral cross section a as follows ... [Pg.979]

The final scattering angle 0 is defined rising 0 = 0(t = oo). There will be a correspondence between b and 0 that will tend to look like what is shown in figure A3.11.5 for a repulsive potential (liere given for the special case of a hard sphere potential). [Pg.995]

Figure A3.11.6. Dependence of scattering angle r on impact parameter for a 6-12 potential. Figure A3.11.6. Dependence of scattering angle r on impact parameter for a 6-12 potential.
Figure Bl.6.8 Energy-loss spectra of 200 eV electrons scattered from chlorine at scattering angles of 3° and 9° [10]. Optically forbidden transitions are responsible for the intensity in the 9° spectrum that does not appear in the 3 ° spectrum. Figure Bl.6.8 Energy-loss spectra of 200 eV electrons scattered from chlorine at scattering angles of 3° and 9° [10]. Optically forbidden transitions are responsible for the intensity in the 9° spectrum that does not appear in the 3 ° spectrum.
This is the Porod law for the large angle tail of the scattering curve in the meridional direction. In this case, the scattered intensity is proportional to -at large scattering angles. [Pg.1406]

Scattering angles =100 keV) Large ( > 10 mrad) Smaller (< 10 mrad)... [Pg.1626]

Figure Bl.17.3. STEM detectors (a) conventional bright and dark-field detectors, electrons are detected according to their different scattering angles, all other positional infonnation is lost (b) positional detector as developed by Haider and coworkers (Haider etal 1994). Figure Bl.17.3. STEM detectors (a) conventional bright and dark-field detectors, electrons are detected according to their different scattering angles, all other positional infonnation is lost (b) positional detector as developed by Haider and coworkers (Haider etal 1994).
A = /W//Wp, P is impact parameter and Tq is the distance of closest approach (apsis) of the collision pair. The transformations from the CM coordinates (scattering angle y) to the laboratory coordinates with the scattering angle 0 for the primary particle and (]) for the recoiled surface atoms Is given by... [Pg.1809]

Figure Bl.23.8. Scattering intensity of 2 keV Ne versus azimuthal angle 6 scans for Pt 110] in the (1 x 2) and (1 X 3) reconstructed phases. Scattering angle 0 = 28° and incident angle a = 6°. Figure Bl.23.8. Scattering intensity of 2 keV Ne versus azimuthal angle 6 scans for Pt 110] in the (1 x 2) and (1 X 3) reconstructed phases. Scattering angle 0 = 28° and incident angle a = 6°.
The scattering and recoil angles 0 and 0g in die Lab frame are related to the CM scattering angle by... [Pg.2008]

The dashed circle denotes the possible laboratory velocities tt for the fidl range of CM scattering angles 9. ... [Pg.2063]


See other pages where Scattering angles is mentioned: [Pg.309]    [Pg.575]    [Pg.872]    [Pg.877]    [Pg.1219]    [Pg.1221]    [Pg.1224]    [Pg.1308]    [Pg.1308]    [Pg.1308]    [Pg.1317]    [Pg.1318]    [Pg.1319]    [Pg.1323]    [Pg.1373]    [Pg.1378]    [Pg.1388]    [Pg.1390]    [Pg.1391]    [Pg.1391]    [Pg.1392]    [Pg.1397]    [Pg.1400]    [Pg.1410]    [Pg.1625]    [Pg.1626]    [Pg.1626]    [Pg.1628]    [Pg.1628]    [Pg.1635]    [Pg.1801]    [Pg.1802]    [Pg.1806]    [Pg.1809]    [Pg.1811]    [Pg.1813]    [Pg.1815]    [Pg.1824]    [Pg.1831]    [Pg.2062]   
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